a.College of Chemistry and Environmental Engineering, Shenzhen University, Shenzhen 518060, China
b.Department of Chemical Physics, University of Science and Technology of China, Hefei 230026, China
lianweili@szu.edu.cn
收稿:2022-07-08,
修回:2022-8-4,
录用:2022-9-14,
网络首发:2022-10-20,
纸质出版:2022-12-01
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Huang, S. Q.; Zhu, M.; Yang, J. X.; Li, L. W. Structural feature and internal motion of hyperbranching cluster system with low polydispersity and featured pattern in dilute solutions. Chinese J. Polym. Sci. 2022, 40, 1515–1521
Si-Qi Huang, Mo Zhu, Jin-Xian Yang, et al. Structural Feature and Internal Motion of Hyperbranching Cluster System with Low Polydispersity and Featured Pattern in Dilute Solutions[J]. Chinese Journal of Polymer Science, 2022, 40(12): 1515-1521.
Huang, S. Q.; Zhu, M.; Yang, J. X.; Li, L. W. Structural feature and internal motion of hyperbranching cluster system with low polydispersity and featured pattern in dilute solutions. Chinese J. Polym. Sci. 2022, 40, 1515–1521 DOI: 10.1007/s10118-022-2864-4.
Si-Qi Huang, Mo Zhu, Jin-Xian Yang, et al. Structural Feature and Internal Motion of Hyperbranching Cluster System with Low Polydispersity and Featured Pattern in Dilute Solutions[J]. Chinese Journal of Polymer Science, 2022, 40(12): 1515-1521. DOI: 10.1007/s10118-022-2864-4.
The reduced first cumulant [
Γ
*
=
Γ
(
q
)/(
q
3
k
B
T
/
η
0
)] for cluster dose not display an asymptotic behaviour
which differs from previously reported behavior of individual chain systems with low polydispersity feature.
This work reports the structural feature and internal motion of one novel hyperbranching cluster system in dilution solution. The cluster system is composed of HB-PS
300
-
g
-P
t
BA
45
hypergraft copolymer chains with uniform subchain
high molar mass and low polydispersity (
M
w
=1.73×10
6
g/mol and
<
M
w
/
M
n
>
≈1.07)
where HB-PS and P
t
BA represent hyperbranched polystyrene core and poly(
tert
-butyl polyacrylate) graft
respectively. In the selective solvent of PS blocks (cyclohexane
T
θ
=34.5 °C)
the aggregation kinetics and structural feature are found to be precisely tunable for assembled clusters by the aggregation temperature (11 °C
<
T
<
17 °C) and time (0 h
<
t
<
24 h). An interesting structural evolution kinetics is observed
namely
the fractal dimension (
d
f
) of clusters is found to first increases and then decreases with
t
eventually
it reaches a plateau value of
d
f
≈3.0
corresponds to a uniform spherical structure. By using dynamic light scattering (DLS) to monitor the number and strength of relaxation modes in
Γ
(
q
) with
Γ
being the decay rate and
q
being the scattering vector
it is quantitatively revealed that the relaxation
intensity contribution and mode origin of internal motions of clusters are neither similar with previously reported cluster systems with high polydispersity
nor with the classical linear chain systems. In particular
in the broad range of 2.0
<
qR
h
<
6.0
we have observed that the reduced first cumulant [
Γ
* =
Γ
(
q
)/(
q
3
k
B
T
/
η
0
)] does not display an asymptotic behavior. Whereas
a better asymptotic behavior is observed by plotting
Γ
(
q
)/
q
4
versus
qR
h
. For the first time
our observation provides direct evidence supporting that
for hyperbranching cluster system with low polydispersity and high local chain segment density
the hydrodynamic interaction is greatly weakened due to the enhanced hydrodynamic shielding effect.
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